{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:HBB6TYJJIDK2OBWVJ42NINKHTJ","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"0e34973141cc8295af838ae1ebbb90ec9dd7c96ea8c32e248d8cfc8b5b4a080b","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2025-07-30T12:40:00Z","title_canon_sha256":"ca0057720b6917a38869deb1125020a20ff53c8c60920dc58a3c9ecccb156970"},"schema_version":"1.0","source":{"id":"2507.22622","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2507.22622","created_at":"2026-07-05T11:45:45Z"},{"alias_kind":"arxiv_version","alias_value":"2507.22622v1","created_at":"2026-07-05T11:45:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2507.22622","created_at":"2026-07-05T11:45:45Z"},{"alias_kind":"pith_short_12","alias_value":"HBB6TYJJIDK2","created_at":"2026-07-05T11:45:45Z"},{"alias_kind":"pith_short_16","alias_value":"HBB6TYJJIDK2OBWV","created_at":"2026-07-05T11:45:45Z"},{"alias_kind":"pith_short_8","alias_value":"HBB6TYJJ","created_at":"2026-07-05T11:45:45Z"}],"graph_snapshots":[{"event_id":"sha256:d34e91411702e9b930a36054507906f8e8c6f9fbb83e426409ab087d8149ba80","target":"graph","created_at":"2026-07-05T11:45:45Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2507.22622/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Light detection and ranging is a key technology for a number of applications, from relatively simple distance ranging to environmental monitoring. When dealing with low photon numbers an important issue is the improvement of the signal- to-noise-ratio, which is severely affected by external sources whose emission is captured by the detection apparatus. In this paper, we present an extension of the technique developed in [Phys. Rev. Lett. 123, 203601] to the effects caused by the propagation of light through a turbulent media, as well as the detection through photon counting devices bearing imp","authors_text":"Ilaria Gianani, Marco Barbieri, Vincenzo Berardi, Walter Zedda","cross_cats":["physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2025-07-30T12:40:00Z","title":"Thresholded quantum LIDAR in turbolent media"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2507.22622","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:4c1f1256dbaa1418d56b720e7fa85bd35494ee569d103d6cb80aeed3095eac4e","target":"record","created_at":"2026-07-05T11:45:45Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"0e34973141cc8295af838ae1ebbb90ec9dd7c96ea8c32e248d8cfc8b5b4a080b","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2025-07-30T12:40:00Z","title_canon_sha256":"ca0057720b6917a38869deb1125020a20ff53c8c60920dc58a3c9ecccb156970"},"schema_version":"1.0","source":{"id":"2507.22622","kind":"arxiv","version":1}},"canonical_sha256":"3843e9e12940d5a706d54f34d435479a75d9eff7c00a253ddda2a3d7c02640cb","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3843e9e12940d5a706d54f34d435479a75d9eff7c00a253ddda2a3d7c02640cb","first_computed_at":"2026-07-05T11:45:45.772793Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:45:45.772793Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"5U55mVGzHroeHnIr1HQMEi+m7thAOJ4g4wLpttBgmFfrgYLVd75LBL/6GYBsr6kfwjQAmmCDoZ3e4B/5oIJiCw==","signature_status":"signed_v1","signed_at":"2026-07-05T11:45:45.773308Z","signed_message":"canonical_sha256_bytes"},"source_id":"2507.22622","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4c1f1256dbaa1418d56b720e7fa85bd35494ee569d103d6cb80aeed3095eac4e","sha256:d34e91411702e9b930a36054507906f8e8c6f9fbb83e426409ab087d8149ba80"],"state_sha256":"5d64c63e067f5542d30caedba1164fbfddeab3c354582a8f0f2e7898e81d9ad2"}